p07_015.pdf

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15. There is no acceleration, so the lifting force is equal to the weight of the object. We note that the
person’s pull
F
is equal (in magnitude) to the tension in the cord.
(a) As indicated in the
hint,
tension contributes twice to the lifting of the canister: 2T =
mg.
Since,
|
F
|
=
T
, we find
|
F
|
= 98 N.
(b) To rise 0.020 m, two segments of the cord (see Fig. 7-28) must shorten by that amount. Thus, the
amount of string pulled down at the left end (this is the magnitude of
d,
the downward displacement
of the hand) is
d
= 0.040 m.
(c) Since (at the left end) both
F
and
d
are downward, then Eq. 7-7 leads to
W
=
F
·
d
= (98)(0.040) =
3.9 J.
(d) Since the force of gravity
F
g
(with magnitude
mg)
is opposite to the displacement
d
c
= 0.020 m
(up) of the canister, Eq. 7-7 leads to
W
=
F
g
·
d
c
=
−(196)(0.020)
=
−3.9
J. This is consistent with
Eq. 7-15 since there is no change in kinetic energy.
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